在 (2+1) 维的Kadomtsev-Petviashvili-Sawada-Kotera-Ramani方程中分析构建和可视化非线性波的稳定性分析
Mahy Ahmed1, Hamdy M Ahmed2, Niveen Badra3
1Department of Physics and Mathematics Engineering, Faculty of Engineering, Ain Shams University, Cairo, Egypt. mahyhashad@eng.asu.edu.eg.
Scientific reports
|September 15, 2025
概括
研究人员探索了 (2+1) 维的Kadomtsev-Petviashvili-Sawada-Kotera-Ramani (KPSKR) 方程,为非线性波现象找到各种精确的分析解决方案. 该研究使用先进的tanh函数方法可视化复杂的波结构和非线性动力学.
科学领域:
- 数学物理 数学物理
- 非线性动力学是一种非线性动力学.
- 波浪现象是一种波浪现象.
背景情况:
- 在 (2+1) 维的Kadomtsev-Petviashvili-Sawada-Kotera-Ramani (KPSKR) 方程模型复杂的非线性波现象.
- 了解这些波对各种科学和工程领域至关重要.
研究的目的:
- 用先进的分析方法研究KPSKR方程.
- 导出和描述各种精确的解决方案.
- 为了可视化非线性波的动态.
主要方法:
- 采用了改进的修改扩展的tanh功能方法.
- 获得了精确的分析解决方案,包括明亮的单子,单一的单子和周期波.
- 利用2D和3D图形可视化来分析波浪行为.
主要成果:
- 成功获得了KPSKR方程的各种精确分析解决方案.
- 确定了明亮的单子子,单一的单子子,单一的周期波和过度的函数解决方案.
- 视觉化揭示了波的复杂的物理特征和动态行为.
结论:
- 改进的修改后扩展的tanh函数方法对于解决复杂的非线性方程是有效的.
- KPSKR方程表现出丰富的非线性动力学,并支持复杂的波形结构.
- 这些发现为在更高维度中非线性波传播提供了宝贵的见解.
相关概念视频
Linear Approximation in Time Domain
347
Nonlinear systems often require sophisticated approaches for accurate modeling and analysis, with state-space representation being particularly effective. This method is especially useful for systems where variables and parameters vary with time or operating conditions, such as in a simple pendulum or a translational mechanical system with nonlinear springs.
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
347
Linear Approximation in Frequency Domain
358
Linear systems are characterized by two main properties: superposition and homogeneity. Superposition allows the response to multiple inputs to be the sum of the responses to each individual input. Homogeneity ensures that scaling an input by a scalar results in the response being scaled by the same scalar.
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
358
Stability
384
The time response of a linear time-invariant (LTI) system can be divided into transient and steady-state responses. The transient response represents the system's initial reaction to a change in input and diminishes to zero over time. In contrast, the steady-state response is the behavior that persists after the transient effects have faded.
The stability of an LTI system is determined by the roots of its characteristic equation, known as poles. A system is stable if it produces a bounded...
The stability of an LTI system is determined by the roots of its characteristic equation, known as poles. A system is stable if it produces a bounded...
384
Equations of Wave Motion
8.3K
Mathematically, the motion of a wave can be studied using a wavefunction. Consider a string oscillating up and down in simple harmonic motion, having a period T. The wave on the string is sinusoidal and is translated in the positive x-direction as time progresses. Sine is a function of the angle θ, oscillating between +A and −A and repeating every 2π radians. To construct a wave model, the ratio of the angle θ and the position x is considered.
8.3K
Multimachine Stability
548
Multimachine stability analysis is crucial for understanding the dynamics and stability of power systems with multiple synchronous machines. The objective is to solve the swing equations for a network of M machines connected to an N-bus power system.
In analyzing the system, the nodal equations represent the relationship between bus voltages, machine voltages, and machine currents. The nodal equation is given by:
In analyzing the system, the nodal equations represent the relationship between bus voltages, machine voltages, and machine currents. The nodal equation is given by:
548
Navier–Stokes Equations
2.1K
For incompressible Newtonian fluids, where density remains constant, stresses show a linear relationship with the deformation rate, defined by normal and shear stresses. Normal stresses depend on the pressure exerted on the fluid and the rate of deformation in specific directions, which determines how fluid flows under varying pressures. Shear stresses, on the other hand, act tangentially across fluid layers. They explain how adjacent fluid layers slide relative to one another, connecting...
2.1K


